Abstract

Transition metal complexes with orbitally degenerate electronic states are geometrically unstable with respect to distortion from idealized symmetry to give structures with non-degenerate electronic states in accord with the Jahn-Teller theorem. This paper examines such distortions for metal complexes of the general type ML n (4 ≤ n ≤ 9) having open-shell electronic configurations. Such distortions can be of the following two types: (i) a classical Jahn-Teller distortion in which the topology of the polyhedron is maintained but the symmetry is lowered from a point group G to a smaller point group K where G is a subgroup of K ; (ii) distortions in which both the topology and symmetry of the polyhedron are changed, typically by diamond-square processes, from a point group G 1 to G 2 where G 2 is not necessarily a subgroup of G 1 . Certain octahedral metal complexes ML 6 deviating from the favored closed-shell 18-electron rare gas electronic configuration are observed to be geometrically unstable to both types of distortions, e.g., elongation of a hyperelectronic O h octahedron to a D 4 h square bipyramid in octahedral d 9 Cu(II) complexes as compared with trigonal twists of hypoelectronic early transition metal dithiolates (e.g., Mo [S 2C 2(CF 3) 2] 3) and hexamethyls (e.g., W(CH 3) 6 and Zr(CH 3) 6 2−) to give D 3 h or C 3 v trigonal prismatic complexes. Open-shell tetrahedral metal complexes may similarly be unstable to both types of distortions, e.g. elongation or compression of opposite edges of a T d tetrahedral complex ML 4 to give a D 2 d disphenoidal complex as compared with a 90° twist of a d 8 tetrahedral complex to give a D 4 h , square planar complex. Similar geometric instabilities of open-shell penta-coordinate metal complexes may be resolved by partial diamond-square distortions to intermediate points along the trigonal bipyramid/square pyramid continuum to remove all of the orbital degeneracies. Analogous diamond-square processes in open-shell superoctahedral complexes ML n ( n = 7, 8, 9) along the pentagonal bipyramid/capped octahedron, bisdisphenoid/square antiprism, and tricapped trigonal prism/capped antiprism continua, respectively, are not sufficient to remove all degeneracies. However, neither hypoelectronic nor hyperelectronic superoctahedral metal complexes are expected to be stable.

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